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Study on calculation method of target strength in waveguide

机译:波导靶力量计算方法研究

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Based on the physical acoustic method (the Kirchhoff's approximation) and planar element method, the problem of the echo intensity of the target in a shallow water waveguide is studied. The physical acoustic method is a kind of high frequency approximate calculation method, which ignores the contribution to the scattering field of the shadow of the target. The planar elements method is a method of surface integral numerical discretization based on the physical acoustic method, which is to approximate the target surface with a large number of small planar polygons (or plates and surfaces). In this paper, the target echo is decomposed into the direct wave, sea surface reflection wave and sea bottom reflection wave. The direct wave is obtained by using the planar elements method directly, which is mono-static scattering. The sea surface and sea bottom reflection wave is analyzed by the mirror image method firstly, and the reflection waves are obtained by using the planar elements method, which include mono-static and bi-static scattering. The total scattering field of the target in an homogeneous wave guide is the summation of all the waves mentioned above. The target strength of the BeTSSi-Sub (Benchmark Target Strength Simulation Submarine) simple submarine in free field, and in a shallow water homogeneous wave guide, are calculated at different directions. The BeTSSi-Sub model is a benchmark model and is created and meshed using Ansys soft. In the computational examples, we suppose that the water depth is 100m, the sea surface is the absolute soft interface, and the bottom is the absolute hard interface. The target strength of a submarine under water 20m to 80m was calculated at 1 kHz. The results show that the echo intensity of the target in a shallow water waveguide is different from that of the free field due to the influence of upper and lower interface, and the echo intensity of the target is continuously changing with the depth of target.
机译:基于物理声学方法(Kirchhoff的近似)和平面元素方法,研究了浅水波导中靶的回波强度的问题。物理声学方法是一种高频近似计算方法,忽略对目标阴影的散射场的贡献。平面元件方法是基于物理声学方法的表面积分数值离散化的方法,其是用大量小平面多边形(或板和表面)近似目标表面。在本文中,目标回波被分解成直波,海面反射波和海底反射波。通过直接使用平面元件方法获得直接波,这是单静态散射。通过镜像方法首先分析海面和海底反射波,并且通过使用平面元件方法获得反射波,其包括单静电和双静态散射。均匀波导中的目标的总散射场是上述所有波的求和。在自由场中的βi-sub(基准目标强度模拟潜艇)简单潜艇的目标强度,以及在不同方向上计算出浅水均匀波导。 Betsi-Sub模型是基准模型,使用ANSYS软件创建和网格。在计算示例中,我们假设水深是100米,海面是绝对软接口,底部是绝对硬接口。在20m至80m下潜水艇的潜艇的目标强度在1 kHz下计算。结果表明,由于上下界面的影响,浅水波导中靶的靶的回波强度与自由场的回声强度不同,并且目标的回波强度随着靶的深度而连续变化。

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